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The Delta N gamma electromagnetic transition form factors G*(M)(q(2)) and G*(E)(q(2))

机译:ΔN伽马电磁跃迁形状因子G *(M)(q(2))和G *(E)(q(2))

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A parameter-free, nonperturbative calculation of the DeltaNgamma electromagnetic transition amplitudes G(M)(*)(q(2)), G(E)(*)(q(2)), and the resonant multipole ratio R-EM(q(2)) equivalent to E-1+(3/2)(q(2)) is performed in terms of the well-known nucleon isovector Sachs form factor G V. Our methods are fully relativistic with conservation of the electromagnetic current guaranteed. We find that G(M)(*)(q(2)) decreases more rapidly than the nucleon dipole form factor when -q(2) greater than or similar to 1 GeV2/c(2) and that R-EM(q(2)) remains small even for very high four-momentum transfer implying that the perturbative QCD prediction R-EM(q(2)) --> 1 is purely asymptotic and is valid only for extremely high q(2). (C) 2004 Elsevier B.V. All rights reserved.
机译:DeltaNgamma电磁跃迁幅度G(M)(*)(q(2)),G(E)(*)(q(2))和共振多极比R-EM(等效于E-1 +(3/2)(q(2))的q(2))是根据众所周知的核子等矢量Sachs形状因子G V执行的。我们的方法在保持电磁电流的同时完全相对论保证。我们发现当-q(2)大于或类似于1 GeV2 / c(2)且R-EM(q)时,G(M)(*)(q(2))的下降速度比核子偶极子形状因子下降更快。 (2))即使对于非常高的四动量传递仍然很小,这意味着微扰QCD预测R-EM(q(2))-> 1纯粹是渐近的,仅对极高的 q(2)有效。 (C)2004 Elsevier B.V.保留所有权利。

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